We begin our simulation by equilibrating the binary mixture in the liquid state at temperature \(T=1.0\) . To prepare the glassy sample, the system is then cooled to the final temperature \(T=0.3\)  below the glass transition temperature \(T_g=0.43\)  with a cooling rate \(10^{-5}\) . For statistical averaging, the whole process is repeated 100 times with different initial realizations. Finally, the glassy sample is sheared along the \(xz\)  plane at a constant shear rate \(\dot{\gamma }=10^{-4}\)  up to \(100 \%\)  strain. During the shear process, the temperature is controlled by dissipative particle dynamics thermostat [1]}. The deformed configurations are saved at chosen strain values \(\dot{\gamma }t\) . The relaxation dynamics of these deformed states are studied by allowing the system to evolve with time (keeping \(\dot{\gamma }t\) ) using MD simulation. The time \(t\)  is reset to zero at the beginning of the relaxation process.
